1. The Predominant Role of Coordination Number in Potassium Channel Selectivity 
Michael Thomas, Dylan Jayatilaka, Ben Corry 
Biophysical Journal 
Volume 93, Issue 8, Pages (October 2007)
DOI: /biophysj
Copyright © 2007 The Biophysical Society Terms and Conditions

2. Figure 1
Structures used in energy calculations. (A) Side and (B) top views of the S2 binding site model extracted from crystallographic data are shown. The ab initio geometry-optimized structure for a cluster of (C) K+ and eight water molecules and (D) Na+ and eight water molecules are shown with the ion-oxygen distances to the coordinating ligands noted.
Biophysical Journal  , DOI: ( /biophysj )
Copyright © 2007 The Biophysical Society Terms and Conditions

3. Figure 2
Ion-exchange free energies determined from MD calculations. The free energies are plotted for the exchange of Na+ and K+ between water and either formaldehyde solvent (♢), the S2 binding site from KcsA with harmonic restraints (●), or the liquid S2 model in which the eight carbonyl ligands forming the S2 binding site can move independently without restraints (■). In each case the partial charge of the carbonyl dipole is altered such that the oxygen and carbon atoms carry equal and opposite charge to change the dipole moment of the coordinating ligands. The partial charge of the carbonyl group in the CHARMM27 force field is noted by the vertical doted line. The ∼5kcal/mol selectivity of the S2 binding site is lost when the ligands have more conformational freedom.
Biophysical Journal  , DOI: ( /biophysj )
Copyright © 2007 The Biophysical Society Terms and Conditions

4. Figure 3
Ion-exchange energies determined from ab initio calculations. The energy of the ion-exchange reactions described in the text is plotted against the number of solvent molecules used to coordinate the ions. Exchange energies are plotted relative to K+, which is taken as 0. Results are obtained with the protein harmonically restrained about the crystal structure using either (A) water or (B) acetonitrile as the solvent, as well as with the protein fixed in the crystal structure using water as the solvent (C). The ion types most favored in the channel fall at the bottom of each plot. (D) The selectivity sequence of the site is indicated in the gas phase, in water, and in acetonitrile (MeCN).
Biophysical Journal  , DOI: ( /biophysj )
Copyright © 2007 The Biophysical Society Terms and Conditions

5. Figure 4
Influence of thermal fluctuations on ion-exchange energies determined from MD simulations. The free energy of the exchange reaction is plotted against the temperature of the simulations when the carbon and nitrogen atoms are held in harmonic constraints about their positions in the crystal structure (●) and structures found by minimizing the protein coordinates with either a K+ (○) or Na+ (▵) in the pore. The size of the RMS thermal fluctuations increases linearly with temperature.
Biophysical Journal  , DOI: ( /biophysj )
Copyright © 2007 The Biophysical Society Terms and Conditions

6. Figure 5
Geometry-optimized structures from ab initio calculations. The structure of the K+/S2 (A) and Na+/S2 (B) structures are shown as determined with harmonic constraints applied to the backbone carbon and nitrogen atoms. The structures determined for K+/(OCH2)8 (C) and Na+/(OCH2)8 (D) calculated with no constraints are also shown, demonstrating that K+ can be coordinated by eight carbonyl ligands with little strain, as can be achieved in S2, whereas Na+ prefers to be coordinated by six ligands, which is not possible in S2. (Note that eightfold coordination of Na+ is higher in energy than sixfold coordination.)
Biophysical Journal  , DOI: ( /biophysj )
Copyright © 2007 The Biophysical Society Terms and Conditions

7. Figure 6
Influence of coordination number and dipole moment on Na+/K+ selectivity in flexible systems. The free energy determined from MD calculations in which K+ surrounded by carbonyl ligands is exchanged with Na+ in bulk water is plotted against the number of carbonyl ligands coordinating the ions. The coordination numbers are constrained by forcing the oxygen atoms on the carbonyl ligands to remain with in a 3.5Å sphere. Four different calculations are made with differing partial charges on the carbonyl ligands as specified beside each curve. Equivalent dipole moments assuming an oxygen-carbon separation of 1.23Å are also shown in brackets. Results for the default partial charge of the carbonyl groups in the CHARMM parameter set are shown by the solid line.
Biophysical Journal  , DOI: ( /biophysj )
Copyright © 2007 The Biophysical Society Terms and Conditions